Plasmon polaritons in photonic metamaterial Fibonacci superlattices

ABSTRACT: We study the properties of plasmon polaritons in one-dimensional photonic metamaterial superlattices resulting from the periodic repetition of a Fibonacci structure. We assume the system made up of positive refraction and metamaterial layers. A Drude-type dispersive response for both the d...

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Autores:
Reyes Gómez, Ernesto Amador
Raigoza Bohórquez, Nicolás Fernando
Cavalcanti, Solange Bessa
de Carvalho, C. A. A.
Oliveira, Luiz Eduardo
Tipo de recurso:
Article of investigation
Fecha de publicación:
2010
Institución:
Universidad de Antioquia
Repositorio:
Repositorio UdeA
Idioma:
eng
OAI Identifier:
oai:bibliotecadigital.udea.edu.co:10495/8400
Acceso en línea:
http://hdl.handle.net/10495/8400
Palabra clave:
Fibonacci
Plasmón
Polaritón
Metamateriales
Metamateriales fotónicos
Rights
openAccess
License
Atribución-NoComercial-SinDerivadas 2.5 Colombia
id UDEA2_bfd87873c809b32b64d1d4114c0a2a6e
oai_identifier_str oai:bibliotecadigital.udea.edu.co:10495/8400
network_acronym_str UDEA2
network_name_str Repositorio UdeA
repository_id_str
dc.title.spa.fl_str_mv Plasmon polaritons in photonic metamaterial Fibonacci superlattices
title Plasmon polaritons in photonic metamaterial Fibonacci superlattices
spellingShingle Plasmon polaritons in photonic metamaterial Fibonacci superlattices
Fibonacci
Plasmón
Polaritón
Metamateriales
Metamateriales fotónicos
title_short Plasmon polaritons in photonic metamaterial Fibonacci superlattices
title_full Plasmon polaritons in photonic metamaterial Fibonacci superlattices
title_fullStr Plasmon polaritons in photonic metamaterial Fibonacci superlattices
title_full_unstemmed Plasmon polaritons in photonic metamaterial Fibonacci superlattices
title_sort Plasmon polaritons in photonic metamaterial Fibonacci superlattices
dc.creator.fl_str_mv Reyes Gómez, Ernesto Amador
Raigoza Bohórquez, Nicolás Fernando
Cavalcanti, Solange Bessa
de Carvalho, C. A. A.
Oliveira, Luiz Eduardo
dc.contributor.author.none.fl_str_mv Reyes Gómez, Ernesto Amador
Raigoza Bohórquez, Nicolás Fernando
Cavalcanti, Solange Bessa
de Carvalho, C. A. A.
Oliveira, Luiz Eduardo
dc.subject.none.fl_str_mv Fibonacci
Plasmón
Polaritón
Metamateriales
Metamateriales fotónicos
topic Fibonacci
Plasmón
Polaritón
Metamateriales
Metamateriales fotónicos
description ABSTRACT: We study the properties of plasmon polaritons in one-dimensional photonic metamaterial superlattices resulting from the periodic repetition of a Fibonacci structure. We assume the system made up of positive refraction and metamaterial layers. A Drude-type dispersive response for both the dielectric permittivity and magnetic permeability of the left-handed material is considered. Maxwell’s equations are solved for oblique incidence by using the transfer-matrix formalism. Our results show that the plasmon-polariton modes are considerably affected by the increasing of the Fibonacci-sequence order of the elementary cell. The loss of the long-range spatial coherence of the electromagnetic field along the growth direction, which is due to the quasiperiodicity of the elementary cell, leads to the splitting of the plasmon-polariton frequencies, resulting in a Cantor-type frequency spectra. Moreover, the calculated photonic dispersion indicates that if the plasma frequency is chosen within the photonic (n(w))=0 gap then the plasmon-polariton modes behave essentially as pure plasmon modes.
publishDate 2010
dc.date.issued.none.fl_str_mv 2010
dc.date.accessioned.none.fl_str_mv 2017-09-28T19:39:47Z
dc.date.available.none.fl_str_mv 2017-09-28T19:39:47Z
dc.type.spa.fl_str_mv info:eu-repo/semantics/article
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dc.identifier.citation.spa.fl_str_mv Reyes Gómez, E. A., Raigoza, N., Cavalcanti, S. B., de Carvalho, C. A. A., & Oliveira, L. E. (2010). Plasmon polaritons in photonic metamaterial Fibonacci superlattices. Physical Review B (Condensed Matter). 81(153101), 1-4. DOI:10.1103/PhysRevB.81.153101
dc.identifier.issn.none.fl_str_mv 0370-2693
dc.identifier.uri.none.fl_str_mv http://hdl.handle.net/10495/8400
dc.identifier.doi.none.fl_str_mv 1873 - 2445 E
identifier_str_mv Reyes Gómez, E. A., Raigoza, N., Cavalcanti, S. B., de Carvalho, C. A. A., & Oliveira, L. E. (2010). Plasmon polaritons in photonic metamaterial Fibonacci superlattices. Physical Review B (Condensed Matter). 81(153101), 1-4. DOI:10.1103/PhysRevB.81.153101
0370-2693
1873 - 2445 E
url http://hdl.handle.net/10495/8400
dc.language.iso.spa.fl_str_mv eng
language eng
dc.relation.ispartofjournalabbrev.spa.fl_str_mv Phys Rev B
dc.rights.*.fl_str_mv Atribución-NoComercial-SinDerivadas 2.5 Colombia
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eu_rights_str_mv openAccess
dc.format.mimetype.spa.fl_str_mv application/pdf
dc.publisher.spa.fl_str_mv The American Physical Society
institution Universidad de Antioquia
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spelling Reyes Gómez, Ernesto AmadorRaigoza Bohórquez, Nicolás FernandoCavalcanti, Solange Bessade Carvalho, C. A. A.Oliveira, Luiz Eduardo2017-09-28T19:39:47Z2017-09-28T19:39:47Z2010Reyes Gómez, E. A., Raigoza, N., Cavalcanti, S. B., de Carvalho, C. A. A., & Oliveira, L. E. (2010). Plasmon polaritons in photonic metamaterial Fibonacci superlattices. Physical Review B (Condensed Matter). 81(153101), 1-4. DOI:10.1103/PhysRevB.81.1531010370-2693http://hdl.handle.net/10495/84001873 - 2445 EABSTRACT: We study the properties of plasmon polaritons in one-dimensional photonic metamaterial superlattices resulting from the periodic repetition of a Fibonacci structure. We assume the system made up of positive refraction and metamaterial layers. A Drude-type dispersive response for both the dielectric permittivity and magnetic permeability of the left-handed material is considered. Maxwell’s equations are solved for oblique incidence by using the transfer-matrix formalism. Our results show that the plasmon-polariton modes are considerably affected by the increasing of the Fibonacci-sequence order of the elementary cell. The loss of the long-range spatial coherence of the electromagnetic field along the growth direction, which is due to the quasiperiodicity of the elementary cell, leads to the splitting of the plasmon-polariton frequencies, resulting in a Cantor-type frequency spectra. Moreover, the calculated photonic dispersion indicates that if the plasma frequency is chosen within the photonic (n(w))=0 gap then the plasmon-polariton modes behave essentially as pure plasmon modes.application/pdfengThe American Physical Societyinfo:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/articlehttp://purl.org/coar/resource_type/c_2df8fbb1https://purl.org/redcol/resource_type/ARTArtículo de investigaciónhttp://purl.org/coar/version/c_970fb48d4fbd8a85Atribución-NoComercial-SinDerivadas 2.5 Colombiainfo:eu-repo/semantics/openAccesshttp://creativecommons.org/licenses/by-nc-nd/2.5/co/http://purl.org/coar/access_right/c_abf2https://creativecommons.org/licenses/by-nc-nd/4.0/FibonacciPlasmónPolaritónMetamaterialesMetamateriales fotónicosPlasmon polaritons in photonic metamaterial Fibonacci superlatticesPhys Rev BPhysical Review B, Particle Physics, Nuclear Physics and Cosmology1481153101LICENSElicense.txtlicense.txtArtículo de investigacióntext/plain; charset=utf-81748http://bibliotecadigital.udea.edu.co/bitstream/10495/8400/5/license.txt8a4605be74aa9ea9d79846c1fba20a33MD55CC-LICENSElicense_urllicense_urltext/plain; charset=utf-849http://bibliotecadigital.udea.edu.co/bitstream/10495/8400/2/license_url4afdbb8c545fd630ea7db775da747b2fMD52license_textlicense_texttext/html; charset=utf-80http://bibliotecadigital.udea.edu.co/bitstream/10495/8400/3/license_textd41d8cd98f00b204e9800998ecf8427eMD53license_rdflicense_rdfapplication/rdf+xml; charset=utf-80http://bibliotecadigital.udea.edu.co/bitstream/10495/8400/4/license_rdfd41d8cd98f00b204e9800998ecf8427eMD54ORIGINALReyesErnesto_2010_PlasmonPolaritonsMetamaterial.pdfReyesErnesto_2010_PlasmonPolaritonsMetamaterial.pdfArtículo de investigaciónapplication/pdf355498http://bibliotecadigital.udea.edu.co/bitstream/10495/8400/1/ReyesErnesto_2010_PlasmonPolaritonsMetamaterial.pdff9c0575a09a73f7cbbb7aba3636a50e9MD5110495/8400oai:bibliotecadigital.udea.edu.co:10495/84002021-05-16 11:46:06.701Repositorio Institucional Universidad de Antioquiaandres.perez@udea.edu.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